U.S. patent number 10,839,843 [Application Number 16/556,691] was granted by the patent office on 2020-11-17 for td detection with enhanced hdis signal.
This patent grant is currently assigned to Headway Technologies, Inc., SAE Magnetics (H.K.) Ltd.. The grantee listed for this patent is Headway Technologies, Inc., SAE Magnetics (H.K.) Ltd.. Invention is credited to Ellis Cha, Soramany Ka, Qinghua Zeng.
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United States Patent |
10,839,843 |
Zeng , et al. |
November 17, 2020 |
TD detection with enhanced HDIs signal
Abstract
A method of operating an HDD having a slider-mounted read/write
head that is configured for dynamic fly-height operation (DFH) and
includes at least one head-disk interference sensor (HDIs). By
operating the DFH to lower the head and subjecting the HDIs signal
to a power-law enhancement, a consistent and accurate determination
of the touchdown power (TDP) can be obtained. Combining absolute
TDP determination with a method for measuring relative changes of
FH, an absolute determination of FH can be determined.
Inventors: |
Zeng; Qinghua (Fremont, CA),
Ka; Soramany (San Jose, CA), Cha; Ellis (San Ramon,
CA) |
Applicant: |
Name |
City |
State |
Country |
Type |
SAE Magnetics (H.K.) Ltd.
Headway Technologies, Inc. |
Shatin
Milpitas |
N/A
CA |
HK
US |
|
|
Assignee: |
SAE Magnetics (H.K.) Ltd.
(Shatin, HK)
Headway Technologies, Inc. (Milpitas, CA)
|
Family
ID: |
1000004305803 |
Appl.
No.: |
16/556,691 |
Filed: |
August 30, 2019 |
Current U.S.
Class: |
1/1 |
Current CPC
Class: |
G11B
5/6076 (20130101); G11B 5/6052 (20130101); G11B
5/4826 (20130101) |
Current International
Class: |
G11B
5/09 (20060101); G11B 5/60 (20060101); G11B
5/48 (20060101) |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Agustin; Peter Vincent
Attorney, Agent or Firm: Saile Ackerman LLC Ackerman;
Stephen B.
Claims
What is claimed is:
1. A method for operating a dynamic flying height (DFH)-configured
read/write head to determine a touchdown power (TDP, or TD power),
comprising: providing a slider-mounted DFH-configured, read/write
head operationally installed in a system wherein said read/write
head is configured to controllably approach the surface of a
rotating recording medium; wherein said slider-mounted
DFH-configured read/write head is mounted on a slider
aerodynamically configured to support said DFH-configured
read/write head at a stable flying height (FH) above a rotating
magnetic recording medium; wherein said slider-mounted read/write
head includes at least one head/disk interference sensor (HDIs) and
associated electronic equipment for receiving and processing
signals generated by said HDIs; wherein said slider-mounted
read/write head further includes DFH apparatus to raise and lower
said slider-mounted read/write head relative to a surface of said
rotating recording medium; generating an HDIs signal, x(t), as
power is applied to said DFH apparatus and said slider-mounted
read/write head approaches said surface of said rotating recording
medium; then enhancing said HDIs signal, x(t), by applying a
power-law signal processing formula to x(t) to obtain y(t):
y(t)=(abs(x(t))){circumflex over ( )}np, np=2, 3, . . . , while
said approach occurs; and determining a TDP using said enhanced
signal y(t).
2. The method of claim 1 wherein said TDP provides an absolute
reference point whereby a method of determining relative changes in
slider height can be combined with said absolute reference point to
create a method to determine a flying height (FH) of said
slider-mounted read/write head.
3. The method of claim 1 wherein in said signal processing formula:
y(t)=(abs(x(t))){circumflex over ( )}np, np=2,3, . . . , np can be
chosen to produce an optimal comparison with an independent
measuring device.
4. The method of claim 3 wherein np is an even integer and the
absolute value of x(t) is its positive value.
5. The method of claim 3 wherein said independent measuring device
is a laser doppler vibrometer (LDV).
6. The method of claim 1 wherein said signal processing further
includes a step of filtering, either before or after said
enhancement of the signal.
7. The method of claim 1 wherein said signal processing further
includes a step of signal amplification either before or after said
enhancement of the signal.
8. The method of claim 1 applied to the manufacture of active HDD
components, said components including a slider and/or a head gimbal
assembly (HGA) and said application occurring during electric or
dynamic electric test (ET, or DET) during manufacturing of said HDD
components (slider and/or HGA).
9. A dynamic flying height (DFH)-configured read/write head having
an absolutely determined touchdown point (TDP), comprising: a
slider-mounted DFH-configured, read/write head operationally
installed in a system wherein said read/write head is configured to
controllably approach the surface of a rotating recording medium;
wherein said slider-mounted DFH-configured read/write head is
mounted on a slider aerodynamically configured to support said
DFH-configured read/write head at a stable flying height (FH) above
a rotating magnetic recording medium; wherein said slider-mounted
DFH-configured read/write head comprises at least one head/disk
interference sensor (HDIs) and associated electronic equipment for
receiving and processing signals generated by said HDIs; wherein
said slider-mounted read/write head further comprises a DFH
apparatus configured to raise and lower said slider-mounted
read/write head relative to a surface of said rotating recording
medium; wherein said HDIs is configured to generate a signal, x(t),
as power is applied to said DFH apparatus and said slider-mounted
read/write head approaches said surface of said rotating recording
medium; wherein said HDIs signal is configured to be processed and
enhanced signal y(t) while said approach occurs and a TDP is
determined using y(t); and wherein said read/write head is
configured to apply the following power-law transformation to said
HDIs signal x(t) to obtain y(t): y(t)=(abs(x(t))){circumflex over (
)}np, np=2, 3, . . . , .
10. The DFH-configured read/write head claim 9 wherein said TDP
provides an absolute reference point wherein, by combining said
absolute TDP with a method of determining relative changes in
slider height a flying height (FH) of said slider-mounted
read/write head is obtained.
11. The DFH-configured read/write head of claim 9 wherein in the
use of the power-law signal processing formula:
y(t)=(abs(x(t))){circumflex over ( )}np, np=2,3, . . . , np can be
chosen to produce an optimal comparison with an independent
measuring device.
12. The DFH-configured read/write head of claim 11 wherein said
independent measuring device is a laser doppler vibrometer
(LDV).
13. The DFH-configured read/write head of claim 9 wherein said
signal processing further includes a step of filtering, either
before or after said enhancement of the signal.
14. The DFH-configured read/write head of claim 9 wherein said
signal processing further includes a step of signal amplification
either before or after said enhancement of the signal.
15. A head-gimbal assembly, comprising: the DFH-configured
read/write head of claim 9; a suspension that elastically supports
said DFH-configured read/write head; a flexure affixed to said
suspension and a load beam having one end attached to said flexure
and another end attached to a base plate.
16. A hard disk drive (HDD), comprising: said head gimbal assembly
of claim 15; a magnetic recording medium positioned opposite to
said DFH-configured read/write head; a spindle motor that rotates
and drives said magnetic recording medium; a device that positions
said DFH-configured read/write head relative to said magnetic
recording medium.
Description
1. TECHNICAL FIELD
This disclosure relates to magnetic write heads that write on
magnetic recording media, particularly to methods of detecting when
a write head makes a contact ("touchdown" or TD) with the surface
of a rotating recording medium.
2. BACKGROUND
Hard disk drives (HDD) have been increasing the recording density
of the magnetic disks on which data storage occurs.
Correspondingly, the thin-film magnetic heads used to write and
read that data have been required to improve their performance as
well. The thin-film read/write heads most commonly in use are of a
composite type, having a structure in which a magnetic-field
detecting device, such as a giant-magnetoresistive (GMR) read
sensor is used together with a magnetic recording device, such as
an inductive electromagnetic coil. These two types of devices are
laminated together and mounted on a rectangular solid prism-shaped
device called a slider. The slider literally flies over the
rotating surface of a disk while being held aloft by aerodynamic
forces at a height called the fly height (FH). The read/write head
is mounted in the slider where it serves to both read and write
data signals, respectively, from and onto magnetic disks which are
the usual magnetic recording media in a HDD.
Typically, the magnetic writer portion of the read/write head is a
small electrically activated coil that induces a magnetic field in
a magnetic pole. The field, in turn, emerges at a narrow write gap
(WG) and can change the direction of the magnetic moments of small
magnetic particles, or groups of particles, embedded in the surface
of the disk. If the embedded particles are embedded in such a way
that their magnetic moments are perpendicular to the disk surface
and can be switched up and down relative to the plane of that
surface, then you have what is called perpendicular magnetic
recording (PMR). The perpendicular arrangement produces a more
densely packed region for magnetic recording.
The constant and rapid increase in the recording area density of
hard disk drives requires a continuous decrease in the flying
height (FH) of the slider, which is the spacing between the
magnetic recording head and disk. After the FH was reduced to about
10 nm, further decrease became extremely difficult to obtain.
Fortunately, at about this time the thermal expansion-based
technique emerged, and it made dynamic flying height (DFH) control
possible. This technique requires that a heating element (heater)
be embedded near the read/write element. When applying electric
power to the heater, it expands thermally and causes the nearby
portion of the read/write element to protrude as well. When this
protrusion occurs, the vertical spacing between the head and the
disk can be reduced locally during reading and writing. This
technology has been widely applied in past several years. As the
recording density just achieved 150 Gbit/cm2 (1 Tbit/in2), the
spacing was decreased to 0.80 or 0.60 nm range.
In order to control the spacing through use of the heater, it is
necessary to have a feasible way of measuring the spacing while
applying the power to the heater. Relative spacing change can be
calculated based on the well-known Wallace equation. However, to
find out the actual spacing, a reference point is required. The
reference point is usually the point where the head touches the
disk, which is then defined as the zero of the spacing. The process
of finding this reference point is called touch down (TD)
detection. Once the reference point is found, the absolute spacing,
which is the spacing relative to the reference point, can be set to
a specified value. This value is typically 0.8 run for current
generation of drives and it is obtained by adjusting the DFH power
during reading and writing.
To obtain better TD detection as well as thermal asperity (TA)
scanning and potential real time FH monitoring, the head element
typically also includes a head-disk interference (HDI) sensor
(HDIs). This sensor is a resistive temperature sensor used to
detect a temperature change in the head that is induced by changes
in clearance during head vibrations or by a direct contact caused
by contact with disk asperities. The HDIs signal has DC and AC
components. During and even after the slider contacts the disk, a
strong high frequency (AC component) HDIs signal might appear. If
the TD vibration is strong, then the AC component of the HDIs
signal can be used to detect the TD. When TD vibration is weak, the
AC signal might be too weak to provide a good detection, in which
case the DC component might provide a better TD detection. However,
in many cases, both AC and DC signals are weak, in which case TD
detection with HDIs signals becomes very challenging.
In some cases, the HDIs signal is strong, but it is sensitive to
the spacing between HDIs and recording media. This spacing has a
large sample-to-sample variation because HDIs protrusion has a
large sample-to-sample variation as a result of the slider
manufacturing process. As a result, there is a large variation of
the TD power detected with HDIs signals. A method is needed to
enhance the HDIs signal so that it is possible to handle these two
kinds of situations.
FIGS. 1A-1D show a complete TD process in an operational system.
FIG. 1A shows a ramping up of DFH power applied to reduce the
spacing between the head and the rotating medium surface. As this
is occurring, FIG. 1B shows the TD vibration on the gimbal (a
portion of the assembly holding the write head as illustrated in
FIG. 9), measured using a laser doppler vibrometer (LDV).
FIGS. 1C and 1D show the HDIs signals captured with different bias
voltages (BHV) on the HDIs detector. The different values of BHV
were used to simulate the HDIs spacing variation effect.
FIGS. 1B, 1C and 1D show that as DFH power increases to bring the
head closer to the rotating medium, both the TD vibration increases
(1B) and HDIs signals increase (1C and 1D) at about 2.0 second or
62 mW. This indicates that a TD occurred around this point.
FIG. 2 shows the RMS of TD vibration and HDIs signals. We observe
that TDP (TD power) detected with TD vibration or with a LDV is
about 62 mW. LDV can detect the true TD, but it can only be used in
a spin-stand component test, and it cannot be used in an actual
HDD. We want to use HDIs to do the TD detection in the HDD.
However, in that case, it is difficult to determine the TDP from
HDIs signals because they are ramping (or not sharp). If we use a
threshold of 0.1 to do the detection, the detected TDP will be
about 58.0 mW with the 280 mV BHV, and about 60.5 mW with the 200
mV BHV. Thus, there are two possibilities:
a) HDIs detection is different from the LDV detection, i.e., it is
not a true TD power;
b) HDIs detection depends on its BHV, i.e., HDIs spacing that has a
large variation. Therefore, HDIs detection is not good although
HDIs signal is strong in this case.
SUMMARY
The first object of this disclosure is to provide a method of
improving TD detection for a slider-mounted read/write head so that
flying height can be more accurately measured and maintained during
HDD operation.
A second object of this disclosure is to provide such a method that
is suitable for application to TD signals that are both very strong
and very weak.
A third object of the present disclosure is to provide such a
method where the detected TD point is very close to the true TD
point.
A fourth object of this disclosure is to provide such a method that
is not sensitive to HDIs spacing so that signals from the HDIs have
a smaller variation.
A fifth object of this disclosure is to provide such a method that
can be implemented under a variety of experimental and operational
conditions, including spin-stand tests, operational HDD use and
slider head gimbal assembly (HGA) electric tests.
The above objects and others as well, will be achieved by a method
that involves processing HDIs signals to enhance them so that the
waveform of the signal is sufficiently well defined that the TD
point can be unambiguously obtained and is the same as that
determined using a detector such as a laser doppler vibrometer
(LDV), which operates on a different principle.
We have demonstrated that, after the HDIs signal is enhanced using
a power-law calculation (operation) as in Eq. 1 below, the RMS
curves become very sharp, as shown FIG. 3. With a large value of
np, detection becomes very easy and consistent.
FIG. 4 shows that with np=10, a substantially identical TDP can be
found from the HDIs signal with a BHV of 280 mV or 200 mV, and it
is very close to the LDV detected TDP. Therefore, detection is
accurate and not sensitive to BHV or HDIs spacing variation.
FIG. 5 shows another case. The HDIs signal is very weak and gentle
(not sharp), and it is very difficult to find TD point from the RMS
plot shown in FIG. 7. However, after the HDIs enhanced with np=10,
the TD signature is very clear in both time history shown in FIG. 6
and RMS curves shown in FIG. 7. Detected TDP with different np were
shown in FIG. 8. In this case, when np>=6, the detected TDP is
consistent and very close to the LDV detection. The method is as
follows.
We begin with a slider-mounted DFH-configured, read/write head
operationally installed in a system such as a HDD or a spin stand
where the read/write head is made to approach the surface of a
rotating recording medium by supplying energy to the DFH mechanism.
The slider-mounted read/write head includes at least one head/disk
interference sensor (HDIs) and associated electronic equipment for
receiving and processing signals generated by said HDIs. The
slider-mounted read/write head also includes a DFH apparatus that
can effectively change the vertical distance between the
slider-mounted read/write head and the surface of the rotating
recording medium. The HDIs generates a signal as power is applied
to the DFH apparatus and the slider-mounted read/write head
approaches the surface of said rotating recording medium. However,
unlike prior art methodologies, the HDIs signal is processed and
enhanced as the approach to TD occurs by transforming the HDIs
signal, x(t), to y(t), which is an enhanced version, specifically,
y(t)=(abs(x(t))){circumflex over ( )}np, np=1, 2, . . . , where the
absolute value of x(t), abs((x(t)) is exponentially raised to an
integer power, np, and amplified and filtered as necessary. This
process makes locating the TD a more exact and reproducible process
and a process that is consistent with other methods of locating the
TD point.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1A is a graphical illustration of the application of DFH
(dynamic flying height) power during a TD process, showing the
stair-like shape of the applied power.
FIG. 1B is a graphical illustration showing a measurement of TD
vibration using an LDV (laser doppler vibrometer) during the TD
process of FIG. 1A.
FIG. 1C is a graphical illustration showing the HDIs signal time
history with a 200 mV BHV (bias voltage) during the TD process of
FIG. 1A.
FIG. 1D is a graphical illustration showing the HDIs signal time
history with a 280 mV BHV during the TD process of FIG. 1A.
FIG. 2 is a set of graphs showing the RMS values of the TD
vibration and HDIs signal of the graphs in FIGS. 1A, B, C and
D.
FIG. 3 is a set of graphs showing the RMS values of HDIs. With
different np values (w/o PE means no signal enhancement)
FIG. 4 is a set of graphs showing the RMS values of the TD
vibration and HDIs signal with np=10.
FIG. 5 is an illustration of the HDIs signal time history before
power enhancement.
FIG. 6 is an illustration of the HDIs signal time history with
np=10.
FIG. 7 is a graph of the RMS value of the HDIs signal with
different np values.
FIG. 8 is a graphical illustration of TDP (TD power) detected using
HDIs with different np values.
FIGS. 9, 10 and 11 are schematic illustration showing the system
incorporated within the components of an operational HDD.
DETAILED DESCRIPTION
The presently disclosed method begins with the use of a
slider-mounted read/write head (the head) configured for dynamic
fly height (DFH) operation, with the head possessing at least one
HDIs (head-disk interference sensor). The head is operationally
installed in a hard disk drive (HDD) or spin-stand wherein it is
allowed to approach the surface of a disk by applying power to the
DFH apparatus and whereby the HDIs produces a signal indicating the
closeness of the approach.
In the present method, however, the HDIs signal is enhanced by
being first subjected to a processing step that raises its absolute
value to an integer power. It will be demonstrated in the following
that the processed signal provides a more accurate and reproducible
indication of the approach than does an unprocessed signal.
Assuming the unprocessed HDIs signal, as a function of time, t, is
denoted x(t), the enhancement transformation y(t), which is a
power-law operation, is applied to it as follows:
y(t)=(abs(x(t))){circumflex over ( )}np, np=2,3, . . . , (1) where
y(t) is the enhanced HDIs signal, abs(x(t)) is the absolute value
of the signal, np is a positive integer, np=1, 2, . . . , and y(t)
is given by equ. (1) above, where (abs(x(t))){circumflex over (
)}np is the exponentiation of the absolute value of x(t) to the
integer power np.
The following brief example will show how the method is
applied:
The typical measured HDIs AC signal includes two portions: noise
and a slider/disk contact signal (or TD signal). If there are n
measurement points in a complete disk revolution and if the slider
contacts the disk at point i (the slider/disk contact usually
starts at a local point), then the measured AC signal will be:
noise(1), noise(2), noise(i)+TD signal(i), noise(+1), . . . ,
noise(n). If we set np=2 in Eq. 1, the transformed signal will
be
noise(1){circumflex over ( )}2, noise(2){circumflex over ( )}2,
[noise(i)+TDsignal(i)]{circumflex over ( )}2, noise(i+1){circumflex
over ( )}2, . . . , noise(n){circumflex over ( )}2. Or
noise(1){circumflex over ( )}2, noise(2){circumflex over ( )}2,
noise(i){circumflex over (
)}2+2*noise(i)*TDsignal(i)+TDsignal(i){circumflex over ( )}2,
noise(i+1){circumflex over ( )}2, . . . , noise(n){circumflex over
( )}2.
Thus, the signal at point i will be enhanced. With a large value of
np, the signal will have more enhancements. That is shown in FIGS.
5 and 6.
The RMS of the enhanced signals will show a larger difference
between before the contact and after the contact, whereby the RMS
curve will have a sharper change around contact point (contact
power) with a larger np, as shown in FIG. 3.
If values of np=2, 4, 6, . . . , are used, there is no need to
calculate absolute value of x(t) (as is shown in Eq. 1). This is
preferred, as it is easier to implement with a hardware circuit. If
odd values of np=3, 5, 7, . . . , are used, the absolute value of
x(t) must be calculated first, and then the power-law calculation
is done.
FIGS. 1A-1D show various aspects of an entire TD process. A ramping
up of DFH power was applied in FIG. 1A, and TD vibration on a
gimbal (see 200 in FIG. 9 for illustration of a gimbal) was
measured in FIG. 1B using a laser doppler vibrometer (LDV). HDIs
signals were captured at different bias voltages (BHV), as shown in
FIG. 1C (BHV=200 mV) and FIG. 1D (BHV=280 mV). The different BHV
values were used to simulate a spacing variation effect of the
HDIs.
As can be seen in the figures, as DFH power increases, both TD
vibration increases (FIG. 1B) and HDIs signals increase until about
2.0 seconds or 62 mW (FIGS. 1C and 1D). This indicates that a TD
occurred at around this point in time.
FIG. 2 shows the RMS of both the TD vibrations and HDIs signals. It
can be seen that the TD power (TDP) detected by TD vibration or by
LDV is about 62.0 mW. Although the LDV can detect the true TD, it
can only be used in a spin-stand component test and it cannot be
used in the HDD. We want to use HDIs to do the TD detection in the
HDD. However, it is difficult to determine the TDP from HDIs
signals because they are ramping (or not sharp). If we use a
threshold 0.1 for the detection, the detected TDP will be about
58.0 mW with the 280 mV BHV, and about 60.5 mW with the 200 mV BHV.
Thus, there are two issues:
a) the 58.0 and 60.5 mW are different from the LDV detection (62.0
mW), or they are not the true TD power;
b) the results depend on BHV, i.e., HDIs spacing that has a large
variation.
Therefore, HDIs detection is not good, even though the HDIs signal
is strong in this case. However, when we enhanced the HDIs with a
power-law calculation (operation) shown in Eq. 1, the RMS curves
become very sharp, as shown in FIG. 3. Using a large value of np in
Eq. 1, detection becomes very easy and consistent.
FIG. 4, which graphs the results of several different np values,
shows that with np=10, an identical TDP can be found when using the
HDIs signal with a BHV of 280 mV or 200 mV, and the value is very
close to LDV detected TDP. Therefore, detection is accurate and not
sensitive to BHV or HDIs spacing variation.
FIG. 5 shows another case. Here, the HDIs signal is very weak and
smooth (not sharp) as compared to FIGS. 1C and 1D, and it is very
difficult to find the TD point from the RMS plot shown in FIG. 7.
However, after the HDIs signal is enhanced with np=10 in Eq. 1, the
TD signature is very clear in both time history shown in FIG. 6 and
RMS curves shown in FIG. 7. Detected TDP with different values of
np are shown FIG. 8. In this case, when np>6, detected TDP is
consistent and very close to the LDV detection.
Referring finally to FIGS. 9, 10 and 11, there is shown an
exemplary magnetic recording apparatus, such as a PMR configured
hard disk drive (HDD), through whose use a PMR read/write head
configured for DFH operation described above will meet the objects
of this disclosure.
FIG. 9 shows a head gimbal assembly (HGA) 200 that includes a
slider-mounted PMR read/write head 100 configured for DFH operation
and having at least one HDIs. A suspension 220 elastically supports
the head 100. The suspension 220 has a spring-like load beam 230
made with a thin, corrosion-free elastic material like stainless
steel. A flexure 231 is provided at a distal end of the load beam
and a base-plate 240 is provided at the proximal end. The head 100
is attached to the load beam 230 at the flexure 230 which provides
the read/write head with the proper amount of freedom of motion. A
gimbal part for maintaining the read/write head at a proper level
is provided in a portion of the flexure 230 to which the read/write
head 100 is mounted.
A member to which the HGA 200 is mounted to arm 260 is referred to
as head arm assembly 220. The arm 260 moves the read/write head 100
in the cross-track direction y across the medium 14 (here, a hard
disk). One end of the arm 260 is mounted to the base plate 240. A
coil 231 to be a part of a voice coil motor is mounted to the other
end of the arm 260. A bearing part 233 is provided to the
intermediate portion of the arm 260. The arm 260 is rotatably
supported by a shaft 234 mounted to the bearing part 233. The arm
260 and the voice coil motor (not shown) that drives the arm 260
configure an actuator.
Referring next to FIG. 10 and FIG. 11, there is shown a head stack
assembly and a magnetic recording apparatus in which the
slider-mounted read/write head 100 is contained. The head stack
assembly is an element to which the HGA 200 is mounted to arms of a
carriage having a plurality of arms. FIG. 10 is a side view of this
assembly and FIG. 11 is a plan view of the entire magnetic
recording apparatus.
A head stack assembly 250 has a carriage 251 having a plurality of
arms 260. The HGA 200 is mounted to each arm 260 at intervals to be
aligned in the vertical direction. A coil 231 (see FIG. 9), which
is to be a portion of a voice coil motor is mounted at the opposite
portion of the arm 260 in the carriage 251. The voice coil motor
has a permanent magnet 263 arranged at an opposite location across
the coil 231.
Referring finally to FIG. 11, the head stack assembly 250 is shown
incorporated into a magnetic recording apparatus 290. The magnetic
recording apparatus 290 has a plurality of magnetic recording media
14 mounted on a spindle motor 261. Each individual recording media
14 has two PMR elements 100 arranged opposite to each other across
the magnetic recording media 14 (shown clearly in FIG. 10). The
head stack assembly 250 and the actuator (except for the read/write
head itself) act as a positioning device and support the PMR heads
100. They also position the PMR heads correctly opposite the media
surface in response to electronic signals. The read/write head
records information onto the surface of the magnetic media by means
of the magnetic pole contained therein.
We wish to point out here that the present method of determining
TD's can be applied not only to an operational HDD, but also to the
fabrication and testing of HDD components such as the head gimbal
assembly (HGA) described above. Moreover, it can also be applied in
electric or dynamics electric test (ET, or DET) during
manufacturing of HDD components (slider and/or HGA, head-gimbal
assembly). During ET or DET, TD detection is required, and the
present method should be very helpful also.
As is understood by a person skilled in the art, the present
description is illustrative of the present disclosure rather than
limiting of the present disclosure. Revisions and modifications may
be made to methods, materials, structures and dimensions employed
in operating a HDD-mounted slider configured for DFH recording that
uses processed signals from an HDIs to ensure that accurate FH
measurements of HDIs can be taken during TDs while still operating
such a device in accord with the spirit and scope of the present
disclosure as defined by the appended claims.
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